JPS62244259A - Permanent magnet type motor - Google Patents
Permanent magnet type motorInfo
- Publication number
- JPS62244259A JPS62244259A JP61085967A JP8596786A JPS62244259A JP S62244259 A JPS62244259 A JP S62244259A JP 61085967 A JP61085967 A JP 61085967A JP 8596786 A JP8596786 A JP 8596786A JP S62244259 A JPS62244259 A JP S62244259A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- rotor
- magnet
- divided
- split
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000004804 winding Methods 0.000 claims 1
- BGPVFRJUHWVFKM-UHFFFAOYSA-N N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] Chemical compound N1=C2C=CC=CC2=[N+]([O-])C1(CC1)CCC21N=C1C=CC=CC1=[N+]2[O-] BGPVFRJUHWVFKM-UHFFFAOYSA-N 0.000 abstract description 3
- 230000004907 flux Effects 0.000 description 15
- 238000010586 diagram Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 239000000853 adhesive Substances 0.000 description 2
- 230000001070 adhesive effect Effects 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 229920006351 engineering plastic Polymers 0.000 description 1
Landscapes
- Permanent Field Magnets Of Synchronous Machinery (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は回転子に永久磁石を備えた永久磁石形電動機の
回転子構造に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Field of Application] The present invention relates to a rotor structure of a permanent magnet motor having a rotor equipped with a permanent magnet.
永久磁石形の電動機の軸トルクの変動(一般にコギング
トルク)をおさえるために、固定子ステ i−タコイル
の極に対して、回転子の永久磁石の磁極をスキュー(傾
斜)させて低減させるものがあり1例えば実開昭59−
53679にも前記スキュー構造をもつ永久磁石形電動
機が記載されている。In order to suppress fluctuations in shaft torque (generally known as cogging torque) of permanent magnet electric motors, the magnetic poles of the rotor's permanent magnets are skewed (tilted) with respect to the poles of the stator stator coil. Yes 1 For example, 1987-
No. 53,679 also describes a permanent magnet type electric motor having the above-mentioned skew structure.
屋根瓦状の分割磁石を有する回転子において。 In a rotor with split magnets in the form of roof tiles.
磁極をスキューすることにより、軸トルク変動をおさえ
ることができるが1分割部石の境界部では磁束密度が急
激に変化するので、電動機効率が悪くなる問題があった
。本発明の目的は、分割磁石の境界部の磁束密度変化を
なくし、電動機効率を上げ、トルク変動をおさえること
にある。By skewing the magnetic poles, fluctuations in shaft torque can be suppressed, but the magnetic flux density changes rapidly at the boundary between the divided stones, resulting in a problem of poor motor efficiency. An object of the present invention is to eliminate changes in magnetic flux density at boundaries between divided magnets, increase motor efficiency, and suppress torque fluctuations.
上記目的は、屋根瓦状の分割磁石の分割部を。 The above purpose is to split the split part of the roof tile-shaped split magnet.
磁極のスキュー量と平行に傾斜させ、スキューを分割部
に設置し、この分割部に磁極の境界を形成することによ
り達成される。This is achieved by tilting the magnetic pole parallel to the amount of skew, placing the skew in the divided part, and forming the boundary of the magnetic pole in this divided part.
屋根瓦状の分割磁石で形成される回転子は、−般に回転
軸に接着剤で数個ずつ固定されて形成される。分割境界
部には、かならず隙間が生じるため、この部分での磁束
密度は低下する。従来はスキューなし電動機においては
、この部分が磁極境界になるよう磁極を形成する構造に
している。磁極をスキューした、分割磁石においては、
分割境界部の隙間のための磁束密度低下はさけられない
が1分割境界部をスキュー量と平行に傾斜させて、従来
同様この分割境界部に磁極境界を形成する構造にするこ
とにより、分割境界部での磁束密度の低下は少なくなる
か、あるいはなくなり、電動機効率を上げ、トルク変動
をおさえることができる。A rotor formed of split magnets in the shape of roof tiles is generally formed by fixing several pieces at a time to a rotating shaft with an adhesive. Since a gap is always created at the division boundary, the magnetic flux density at this portion is reduced. Conventionally, a skewless motor has a structure in which the magnetic poles are formed such that this portion becomes the magnetic pole boundary. In a split magnet with skewed magnetic poles,
Although a decrease in magnetic flux density due to the gap at the dividing boundary cannot be avoided, by slanting one dividing boundary parallel to the skew amount and forming a magnetic pole boundary at this dividing boundary as in the conventional structure, the dividing boundary can be reduced. The decrease in magnetic flux density at the end of the motor is reduced or eliminated, increasing motor efficiency and suppressing torque fluctuations.
以下、本発明の一実施例を第1図ないし第4図に示す。 An embodiment of the present invention is shown in FIGS. 1 to 4 below.
第1図は本発明の永久磁石形電動機の構造を示す半断面
図、第2図は第1図の永久磁石を取付した構造を示す回
転子部の斜視図、第3図は第2図の回転子の分割磁石の
配置を示す展開図と回転子中央部A表面の1回転筒II
(360” )の磁束密度波形図で、(a)は展開図
、(b)は磁束密度波形図、第4図は1分割磁石の形状
を示す斜視図である。第1図において、出力軸1は軸受
8により支承されており、かつカラー9、永久磁石5、
相切替用磁石3を保持し、回転子を構成する。ステータ
コア4には、コイル6が巻装され、ステータコア4はエ
ンドブラケット10に固定されている。2は前記相切替
用磁石3に対応して、エンドブラケット10に固定され
ているホール素子27はフレームでこれらは組合せられ
て固定子を形成する。ホール素子2はコイル6に通電を
規則正しく行う為の位置検出を行うものである。第2図
は第1図の回転子部の構造を示す図である。Fig. 1 is a half-sectional view showing the structure of the permanent magnet type electric motor of the present invention, Fig. 2 is a perspective view of the rotor section showing the structure in which the permanent magnets shown in Fig. Developed view showing the arrangement of divided magnets of the rotor and one-turn cylinder II on the surface of rotor central part A
(360"), in which (a) is a developed view, (b) is a magnetic flux density waveform diagram, and Figure 4 is a perspective view showing the shape of a one-divided magnet. In Figure 1, the output shaft 1 is supported by a bearing 8, and includes a collar 9, a permanent magnet 5,
It holds the phase switching magnet 3 and constitutes a rotor. A coil 6 is wound around the stator core 4, and the stator core 4 is fixed to an end bracket 10. 2 corresponds to the phase switching magnet 3, and a Hall element 27 fixed to the end bracket 10 is a frame, which is combined to form a stator. The Hall element 2 is used to detect the position of the coil 6 in order to regularly energize it. FIG. 2 is a diagram showing the structure of the rotor section of FIG. 1.
そして分割磁石5a* 5b* 5c、5dは、カラー
9に接着剤で固定し、分割位置の、■。Then, the divided magnets 5a*, 5b*, 5c, and 5d are fixed to the collar 9 with adhesive, and the divided magnets 5a*, 5b*, 5c, and 5d are placed at the dividing position.
O,■は、それぞれ、磁極境界になるように構成し、着
磁スキュー量θと一致するよう傾斜する構造になってい
る6回転子構造を展開して示すと第3図の(a)になる
、また回転子中央部A部の表面磁束分布波形を示すと第
3図(b)になり、従来問題になったスキュー量θをつ
けた時の分割位置での磁束密度の落ち込み、すなおち第
6図、(c)、(d)の■′、■′・○′・■′位置で
の密度の変化がなくなる。第4図は、第2図の分割磁石
5dの1分割磁石の形状を示した斜視図で、分割位置@
* O端面は、磁極スキュー量θと一致させて傾斜さ
せ、この部分で磁極境界を形成したことを示す、第5図
から第7図に従来の回転子構造を示す。第5図は分割磁
石5a’5b’ 、5c’ 、5d’ において磁極ス
キュー量θを形成する様、着磁したことを示す回転子の
斜視図で、の′、■′、O′、O′は1分割位置である
。この回転子の構造を展開して示すと、第6図(c)に
なる、第6図(d)は回転子中央部表面B部の磁束分布
波形図で、分割位置の′、■′、0′、 ■′で磁束
が落ち込み、電動機の効率が低下する要因となっていた
。Figure 3 (a) shows a developed six-rotor structure in which O and ■ are configured to be magnetic pole boundaries, respectively, and are tilted to match the magnetization skew amount θ. Also, the surface magnetic flux distribution waveform of the central part A of the rotor is shown in Figure 3 (b), which shows that the magnetic flux density drops at the split position when the skew amount θ is set, which has been a problem in the past. There is no change in density at the positions ■', ■', ○', and ■' in FIGS. 6, (c) and (d). FIG. 4 is a perspective view showing the shape of one divided magnet of the divided magnet 5d in FIG.
* The conventional rotor structure is shown in FIGS. 5 to 7, which show that the O end face is inclined to match the magnetic pole skew amount θ, and a magnetic pole boundary is formed at this portion. FIG. 5 is a perspective view of the rotor showing that the divided magnets 5a', 5b', 5c', and 5d' are magnetized so as to form the magnetic pole skew amount θ. is the 1 division position. When the structure of this rotor is developed and shown, it is shown in Fig. 6(c). Fig. 6(d) is a magnetic flux distribution waveform diagram at part B of the rotor's central surface. At 0' and 2', the magnetic flux drops, which causes a decrease in the efficiency of the motor.
第7図は、第5図の分割磁石5d’の1分割磁石の形状
を示した斜視図で、スキュー量θは分割磁石5d’の中
央部に配置され、磁極が着磁されて回転子を形成する1
本発明によれば、分割磁石を分割位置で、着磁スキュー
量0と一致させて傾斜させ、この部分に着磁磁極の境界
を形成させることにより、スキュー量θ付近の軸トルク
変動が小さくなり、磁束密度波形を安定させ、効率の良
い永久磁石形電動機を得ることができるものである。FIG. 7 is a perspective view showing the shape of one divided magnet of the divided magnet 5d' in FIG. form 1
According to the present invention, the shaft torque fluctuation near the skew amount θ is reduced by tilting the split magnets at the split position so as to match the magnetization skew amount of 0 and forming the boundaries of the magnetized magnetic poles at this portion. , it is possible to stabilize the magnetic flux density waveform and obtain an efficient permanent magnet motor.
以上述べたように本発明によれば1分割磁石に、 磁
極スキュー量θを形成しても、軸トルク変動をおさえる
ことができ、しかも、分割位置での磁束密度の落ち込み
をなくすことが出来るので、電動機の効率が向上すると
いう効果を有するものである。As described above, according to the present invention, even if the magnetic pole skew amount θ is formed in the one-segment magnet, it is possible to suppress the shaft torque fluctuation, and moreover, it is possible to eliminate the drop in magnetic flux density at the split position. , which has the effect of improving the efficiency of the electric motor.
第1図は本発明の一実施例を示す永久磁石形電動機の半
断面図、第2図はその回転子の構造を示す斜視図、第3
図は第2図の回転子磁石の展開状態と回転子中央部A表
面の磁束密度分布図の関係図、第4図は一つの分割磁石
斜視図、第5図は従来の回転子構造を示す斜視図、第6
図は第5図の回転子磁石の展開状態と回転子中央部8表
面の磁東密度分布の関係図、第7図は従来の一つの分割
磁石の斜視図である。
1・・・出力軸、2・・・ホール素子、3・・・相切替
用磁石。
4・・・ステータコア、5・・・永久磁石、5a・・・
分割磁石、5b・・・分割磁石、5c・・・分割磁石、
5d・・・分割磁石、5a’・・・分割磁石、5b′・
・・分割磁石、5c’・・・分割磁石、5d’・・・分
割磁石、6・・・コイル、7・・・フレーム、8・・・
軸受、9・・・カラー、10・・・エンプラ、A・・・
回転子表面中央部、B・・・回転子表面中央部、■・・
・分割位置、■・・・分割位置、■・・分割位置、■・
・・分割位置、■邑・・分割位置、■′・・・分割位置
、■′・・・分割位置、■−・・分割位置、0・・・ス
キュー角度、N1・・・磁極、NZ・・・磁極、St・
・・磁極、Sz・・・磁極、(、)・・展開図、(b)
・・・磁束密度分布図、(c)・・・展開図、(d)
・・磁束密度分布図。FIG. 1 is a half-sectional view of a permanent magnet type electric motor showing one embodiment of the present invention, FIG. 2 is a perspective view showing the structure of its rotor, and FIG.
The figure shows the relationship between the developed state of the rotor magnets in Fig. 2 and the magnetic flux density distribution diagram on the surface of the rotor central part A, Fig. 4 is a perspective view of one divided magnet, and Fig. 5 shows the conventional rotor structure. Perspective view, No. 6
The figure shows the relationship between the developed state of the rotor magnets in FIG. 5 and the magnetic east density distribution on the surface of the rotor central portion 8, and FIG. 7 is a perspective view of one conventional divided magnet. 1... Output shaft, 2... Hall element, 3... Phase switching magnet. 4... Stator core, 5... Permanent magnet, 5a...
Divided magnet, 5b...Divided magnet, 5c...Divided magnet,
5d...Divided magnet, 5a'...Divided magnet, 5b'.
... Divided magnet, 5c'... Divided magnet, 5d'... Divided magnet, 6... Coil, 7... Frame, 8...
Bearing, 9...Color, 10...Engineering plastic, A...
Center part of rotor surface, B... Center part of rotor surface, ■...
・Divide position, ■...Divide position, ■...Divide position, ■・
・・Division position, ■・・・・Division position, ■′・・・・・Division position, ■′・・・・Split position, ■−・・・Split position, 0・・Skew angle, N1・・Magnetic pole, NZ・...Magnetic pole, St.
...Magnetic pole, Sz...Magnetic pole, (,)...Development view, (b)
...Magnetic flux density distribution diagram, (c)...Development diagram, (d)
...Magnetic flux density distribution map.
Claims (1)
着したフレームと、このフレーム片方、又は両側に配し
た軸受と、この軸受により回転自在に支承された回転軸
と、この回転軸に固定され、かつ永久磁石を磁極として
備えた回転子とを有するものにおいて、磁極をスキュー
した永久磁石を設けるとともに、永久磁石を分割位置で
スキュー量と等しく傾斜させて、この分割位置に磁極境
界を形成したことを特徴とする永久磁石形電動機。1. A stator core around which a winding is wound, a frame to which this stator core is fixed, a bearing placed on one or both sides of this frame, a rotating shaft rotatably supported by this bearing, and this rotation. In a rotor that is fixed to a shaft and has a rotor with permanent magnets as magnetic poles, permanent magnets with skewed magnetic poles are provided, and the permanent magnets are tilted at divided positions equal to the skew amount, and the magnetic poles are installed at the divided positions. A permanent magnet electric motor characterized by forming a boundary.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61085967A JPS62244259A (en) | 1986-04-16 | 1986-04-16 | Permanent magnet type motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61085967A JPS62244259A (en) | 1986-04-16 | 1986-04-16 | Permanent magnet type motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62244259A true JPS62244259A (en) | 1987-10-24 |
Family
ID=13873501
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61085967A Pending JPS62244259A (en) | 1986-04-16 | 1986-04-16 | Permanent magnet type motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62244259A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6462452B2 (en) * | 2000-05-25 | 2002-10-08 | Mitsubishi Denki Kabushiki Kaisha | Permanent magnet motor |
US6853105B2 (en) | 2000-05-25 | 2005-02-08 | Mitsubishi Denki Kabushiki Kaisha | Permanent magnet motor |
JP2009169924A (en) * | 2007-12-18 | 2009-07-30 | Nippon Telegr & Teleph Corp <Ntt> | Characteristic keyword detection device, characteristic keyword detecting method, program and recording medium |
-
1986
- 1986-04-16 JP JP61085967A patent/JPS62244259A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6462452B2 (en) * | 2000-05-25 | 2002-10-08 | Mitsubishi Denki Kabushiki Kaisha | Permanent magnet motor |
US6853105B2 (en) | 2000-05-25 | 2005-02-08 | Mitsubishi Denki Kabushiki Kaisha | Permanent magnet motor |
US6876116B2 (en) | 2000-05-25 | 2005-04-05 | Mitsubishi Denki Kabushiki Kaisha | Permanent magnet motor |
JP2009169924A (en) * | 2007-12-18 | 2009-07-30 | Nippon Telegr & Teleph Corp <Ntt> | Characteristic keyword detection device, characteristic keyword detecting method, program and recording medium |
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